Using the PDG 22 compilation of the e+e−→ Hadrons ⊕ the recent CMD3 data for the pion form factor and the value of gluon condensate 〈αsG2〉 from heavy quarkonia, we extract the value of the four-quark condensate: ραs〈ψ¯ψ〉2=(5.98±0.64)×10−4 GeV6 and the dimension eight condensate: d8=(4.3±3.0)×10−2 GeV8 from the ratio R10 of Laplace sum rules to order αs4. We show the inconsistency in using at the same time the standard SVZ value of the gluon and the vacuum saturation of the four-quark condensates. Using the previous values of the four-quark and d8 condensates, we re-extract 〈αsG2〉 from R10 to be: (6.12±0.61)×10−2 GeV4 in perfect agreement with the one from heavy quarkonia. We also use the lowest τ-like decay moment Rτee to extract the value of the QCD coupling. We obtain to O(αs4) the mean of FO (fixed order) and CI (contour improved) PT series within the standard OPE: αs(Mτ)=0.3385(50)(136)syst where the last error is an added conservative systematic from the distance of the mean to the FO and CI central values. Assuming that the αs-coefficients of the PT series grow geometrically as observed in the calculated case, we obtain to O(αs5): αs(Mτ)=0.3262(37)(78)syst. These results lead to: αs(MZ)=0.1207(17)(3) [resp. 0.1193(11)(3)] to order αs4 [resp. αs5]. The corresponding value of the sum of the non-perturbative contribution at Mτ is: δNPV(Mτ)=(2.3±0.2)×10−2. Reciprocally, using αs(Mτ), 〈αsG2〉 and d8 as inputs, we test the stability of the value of the four-quark condensate obtained from the lowest τ-like moment. We complete our analysis by updating our previous determinations of the lowest order hadronic vacuum polarization contributions to the lepton anomalies and to α(MZ2). We obtain in Table 3: aμ|l.ohvp=(7036.5±38.9)×10−11, aτ|l.ohvp=(3494.8±24.7)×10−9 and α(5)(MZ)|had=(2766.3±4.5)×10−5. This new value of aμ leads to: Δaμ≡aμexp−aμth=(142±42th±41exp)×10−11 which reduces the tension between the SM prediction and experiment.